Topological quantum phase transition between Fermi liquid phases in an Anderson impurity model
arXiv:1805.11518 · doi:10.1103/PhysRevB.98.195435
Abstract
We study a generalized Anderson model that mixes two localized configurations --one formed by two degenerate doublets and the other by a triplet with single-ion anisotropy -- by means of two degenerate conduction channels. The model has been derived for a single Ni impurity embedded into an O-doped Au chain. Using the numerical renormalization group, we find a topological quantum phase transition, at a finite value between two regular Fermi liquid phases of high (low) conductance and topological number (-1) for (), where is the well-known Luttinger integral. At finite temperature the two phases are separated by a non-Fermi liquid phase with fractional impurity entropy and other properties which remind those of the two-channel Kondo model.
6 pages + Supplemental Material, 8 figures
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- Topological quantum phase transition in individual Fe Atoms on MoS/Au(111)
- The Weyl-Mott point: topological and non-Fermi liquid behavior from an isolated Green's function zero
- Quantum entanglement in a pure state of strongly correlated quantum impurity systems
- Topological charge excitations and Green's function zeros in paramagnetic Mott insulators